{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:ZY73WXW7GWHETI5LGTVMM6IVW7","short_pith_number":"pith:ZY73WXW7","canonical_record":{"source":{"id":"1601.05369","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2016-01-20T18:49:53Z","cross_cats_sorted":[],"title_canon_sha256":"c39c34d24167f45d54919b510db680380b95089c3bb59ec1bb6987bd59ec901d","abstract_canon_sha256":"42b873fd238c5a7d22abd4802417d7b1475cf13a6384c349e42cd7fd29154de0"},"schema_version":"1.0"},"canonical_sha256":"ce3fbb5edf358e49a3ab34eac67915b7f18e3396c4c5d87183a40d2e55fc3b8b","source":{"kind":"arxiv","id":"1601.05369","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1601.05369","created_at":"2026-05-18T01:22:15Z"},{"alias_kind":"arxiv_version","alias_value":"1601.05369v1","created_at":"2026-05-18T01:22:15Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1601.05369","created_at":"2026-05-18T01:22:15Z"},{"alias_kind":"pith_short_12","alias_value":"ZY73WXW7GWHE","created_at":"2026-05-18T12:30:55Z"},{"alias_kind":"pith_short_16","alias_value":"ZY73WXW7GWHETI5L","created_at":"2026-05-18T12:30:55Z"},{"alias_kind":"pith_short_8","alias_value":"ZY73WXW7","created_at":"2026-05-18T12:30:55Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:ZY73WXW7GWHETI5LGTVMM6IVW7","target":"record","payload":{"canonical_record":{"source":{"id":"1601.05369","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2016-01-20T18:49:53Z","cross_cats_sorted":[],"title_canon_sha256":"c39c34d24167f45d54919b510db680380b95089c3bb59ec1bb6987bd59ec901d","abstract_canon_sha256":"42b873fd238c5a7d22abd4802417d7b1475cf13a6384c349e42cd7fd29154de0"},"schema_version":"1.0"},"canonical_sha256":"ce3fbb5edf358e49a3ab34eac67915b7f18e3396c4c5d87183a40d2e55fc3b8b","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:22:15.324742Z","signature_b64":"xCPmbjoK3vmbIxl3JyqCEvBy4fleOI8BYsvTsly1nTb/bRlhxmXn86KEV6j7HsioojZl3YG2EKIDZAKwCoYhDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ce3fbb5edf358e49a3ab34eac67915b7f18e3396c4c5d87183a40d2e55fc3b8b","last_reissued_at":"2026-05-18T01:22:15.324140Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:22:15.324140Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1601.05369","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:22:15Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"DZvgripuz5/1VXb/q/vVqLB+CoRI5Ph19MDgnjOyHoMiaabN920Abn0P+pLEaa4Z9PEHSmGTUS2r6Y4L3+BMDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T11:41:14.992614Z"},"content_sha256":"43c418fb2ac60d1a102e513ab0e4aa33c051f2f2038c48e8d6f16d958a996304","schema_version":"1.0","event_id":"sha256:43c418fb2ac60d1a102e513ab0e4aa33c051f2f2038c48e8d6f16d958a996304"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:ZY73WXW7GWHETI5LGTVMM6IVW7","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Hall quantization and optical conductivity evolution with variable Berry phase in $\\alpha$-$T_3$ model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"E. Illes, E. J. Nicol, J. P. Carbotte","submitted_at":"2016-01-20T18:49:53Z","abstract_excerpt":"The $\\alpha$-$T_3$ model is characterized by a variable Berry phase that changes continuously from $\\pi$ to $0$. We take advantage of this property to highlight the effects of this underlying geometrical phase on a number of physical quantities. The Hall quantization of the two limiting cases is dramatically different - a relativistic series is associated with a Berry phase of $\\pi$ and a non-relativistic series is associated with the other limit. We study the quantization of the Hall plateaux as they continuously evolve from a relativistic to a non-relativistic regime. Additionally, we descri"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1601.05369","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:22:15Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"QonnLM8u8qDX3X40FZsQxDyDjf/Lxy7pG46MN+5xC72Y6EV0pq1Y7PXHC4XB7bJtcx18nU5RSsjwGufZJ3FXBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T11:41:14.992968Z"},"content_sha256":"fcc599ef8f64abd10a6c98d34def673e56de26737e5548b980dc786f07be26b4","schema_version":"1.0","event_id":"sha256:fcc599ef8f64abd10a6c98d34def673e56de26737e5548b980dc786f07be26b4"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/ZY73WXW7GWHETI5LGTVMM6IVW7/bundle.json","state_url":"https://pith.science/pith/ZY73WXW7GWHETI5LGTVMM6IVW7/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/ZY73WXW7GWHETI5LGTVMM6IVW7/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-06-01T11:41:14Z","links":{"resolver":"https://pith.science/pith/ZY73WXW7GWHETI5LGTVMM6IVW7","bundle":"https://pith.science/pith/ZY73WXW7GWHETI5LGTVMM6IVW7/bundle.json","state":"https://pith.science/pith/ZY73WXW7GWHETI5LGTVMM6IVW7/state.json","well_known_bundle":"https://pith.science/.well-known/pith/ZY73WXW7GWHETI5LGTVMM6IVW7/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:ZY73WXW7GWHETI5LGTVMM6IVW7","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"42b873fd238c5a7d22abd4802417d7b1475cf13a6384c349e42cd7fd29154de0","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2016-01-20T18:49:53Z","title_canon_sha256":"c39c34d24167f45d54919b510db680380b95089c3bb59ec1bb6987bd59ec901d"},"schema_version":"1.0","source":{"id":"1601.05369","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1601.05369","created_at":"2026-05-18T01:22:15Z"},{"alias_kind":"arxiv_version","alias_value":"1601.05369v1","created_at":"2026-05-18T01:22:15Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1601.05369","created_at":"2026-05-18T01:22:15Z"},{"alias_kind":"pith_short_12","alias_value":"ZY73WXW7GWHE","created_at":"2026-05-18T12:30:55Z"},{"alias_kind":"pith_short_16","alias_value":"ZY73WXW7GWHETI5L","created_at":"2026-05-18T12:30:55Z"},{"alias_kind":"pith_short_8","alias_value":"ZY73WXW7","created_at":"2026-05-18T12:30:55Z"}],"graph_snapshots":[{"event_id":"sha256:fcc599ef8f64abd10a6c98d34def673e56de26737e5548b980dc786f07be26b4","target":"graph","created_at":"2026-05-18T01:22:15Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"The $\\alpha$-$T_3$ model is characterized by a variable Berry phase that changes continuously from $\\pi$ to $0$. We take advantage of this property to highlight the effects of this underlying geometrical phase on a number of physical quantities. The Hall quantization of the two limiting cases is dramatically different - a relativistic series is associated with a Berry phase of $\\pi$ and a non-relativistic series is associated with the other limit. We study the quantization of the Hall plateaux as they continuously evolve from a relativistic to a non-relativistic regime. Additionally, we descri","authors_text":"E. Illes, E. J. Nicol, J. P. Carbotte","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2016-01-20T18:49:53Z","title":"Hall quantization and optical conductivity evolution with variable Berry phase in $\\alpha$-$T_3$ model"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1601.05369","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:43c418fb2ac60d1a102e513ab0e4aa33c051f2f2038c48e8d6f16d958a996304","target":"record","created_at":"2026-05-18T01:22:15Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"42b873fd238c5a7d22abd4802417d7b1475cf13a6384c349e42cd7fd29154de0","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2016-01-20T18:49:53Z","title_canon_sha256":"c39c34d24167f45d54919b510db680380b95089c3bb59ec1bb6987bd59ec901d"},"schema_version":"1.0","source":{"id":"1601.05369","kind":"arxiv","version":1}},"canonical_sha256":"ce3fbb5edf358e49a3ab34eac67915b7f18e3396c4c5d87183a40d2e55fc3b8b","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ce3fbb5edf358e49a3ab34eac67915b7f18e3396c4c5d87183a40d2e55fc3b8b","first_computed_at":"2026-05-18T01:22:15.324140Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:22:15.324140Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"xCPmbjoK3vmbIxl3JyqCEvBy4fleOI8BYsvTsly1nTb/bRlhxmXn86KEV6j7HsioojZl3YG2EKIDZAKwCoYhDg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:22:15.324742Z","signed_message":"canonical_sha256_bytes"},"source_id":"1601.05369","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:43c418fb2ac60d1a102e513ab0e4aa33c051f2f2038c48e8d6f16d958a996304","sha256:fcc599ef8f64abd10a6c98d34def673e56de26737e5548b980dc786f07be26b4"],"state_sha256":"d0c5fe9b86177c88b1f18c1d0d4bd7e10c22b9fb29f22e115363ab900fa6a8ce"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"1uEsGFPg7s3GivGDfvJVFlId7n63elRNGANzGYUi/DDzPVzVtJRZ0LjwvWMxGpn6aaWeODzhZENSatwbvuoCCA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T11:41:14.994987Z","bundle_sha256":"d7eb06dbf4980b9e2e59369b70e2fca5c17ab327cdce7c8794ff2e09581dddda"}}